Discharge from the pumping well.
Ability of the aquifer to transmit water. Higher T gives a shallower, wider cone.
Aquifer storage coefficient. Smaller S lets the effect spread faster and farther.
Distance from the pumping well. Shown by the green vertical line.
The animation pumps up to this elapsed time.
Scrub the elapsed pumping time back and forth.
Blue = water table; the funnel-shaped drawdown develops as pumping continues. The green vertical line marks the observation well at distance r, and the white dot shows its drawdown.
$s=\frac{Q}{4\pi T}\,W(u),\qquad u=\frac{r^2S}{4Tt}$
$W(u)=-\gamma-\ln u+\sum_{n=1}^{\infty}\frac{(-1)^{n+1}u^{n}}{n\cdot n!}=\int_{u}^{\infty}\frac{e^{-x}}{x}\,dx$
$s$ = drawdown [m], $Q$ = pumping rate, $T$ = transmissivity, $S$ = storage coefficient, $r$ = distance, $t$ = time, $\gamma\approx0.5772$ (Euler constant). $W(u)$ is the well function (exponential integral $E_1$). Smaller $u$ (longer time, closer distance) means larger drawdown. The influence radius is roughly $R\approx\sqrt{4Tt/S}$. The Theis solution assumes a homogeneous confined aquifer, radial flow, and a constant pumping rate; boundaries, leakage, unconfined storage, and well loss need other models.